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Differential scattering cross-section normalized

Gs°(r, t) and Gsc(r, t) determine the incoherent differential scattering cross section for slow neutrons from CO through a weighted sum of their space-time Fourier transforms. Each of these functions is normalized to unity when integrated over all space. [Pg.141]

K) (a) optical micrograph of the related unfunctiO-nalized polymer blend (b). The scattering vector, qx (41T/X) sin (0/2) where 0 is the observation angle. dS/dn is the differential scattering cross-section per atom with respect to the solid angle, as normalized to a unit volume. [Pg.60]

In the limit of assumption (b), the applicability of classical mechanics is normally limited to specific quantities, one of which is the differential scattering cross-section, dcr(6lc), where 0C is the center-of-mass (CM) scattering angle. [Pg.24]

It has already been mentioned in Section 1.2.1 that the term intensity will be used to denote the differential scattering cross section dcr/dQ, i.e., the ratio J(q)IJo. The normalized amplitude defined here is therefore related to the intensity by I(q) = A(q) 2. [Pg.23]

For the special case, then, of plane waves normalized to the box i , Eq. (140) gives the relation between the differential scattering cross-section and the transition probability w of Eq. (138), so that we have derived... [Pg.42]

The primary experimental information from a molecular beam experiment is the fraction of the molecules in the incident beam that is scattered into a particular direction. The fraction is normally expressed in terms of d/, the rate at which molecules are scattered into a cone that represents the area covered by the eye of the detector (Fig. 18.14 of the text). This rate is reported as the differential scattering cross-section, <7. the constant of proportionality between the value of d/ and the intensity, 1, of the incident beam, the number density of target molecules, N, and the infinitesimal path length dr through the sample ... [Pg.358]

Figure 7.13 shows the SAXS differential scattering cross section of normal (proto-nated or H-labeled) polyethylene (PEH) after quenching from the melt [22], The background due to Compton scattering is virtually zero in this Q-range [50] and the SAXS signal arises from fluctuations in density [66, 69]. The interlamellar... [Pg.449]

In this technique, normally incident plane-polarised light is scattered by thin films ( 20 pm thickness) of nematic aligned with the director either parallel or perpendicular to the incident light direction. The scattered light is detected as a function of angle, and for different polarisations of the incident (i) and scattered (f) beams. The differential scattering cross-section per unit volume is given by [12] ... [Pg.166]

To verify the accuracy of the code for isotropic, chiral particles, we consider a spherical particle of size parameter k a = 10. The refractive index of the particle is m-r = 1.5 and the chirality parameter is [3k = 0.1, where ki = m ks. Calculations are performed for A rank = 18 and A int = 200. Figure 3.7 compares the normalized differential scattering cross-sections computed with the... [Pg.203]

Fig. 3.6. Normalized differential scattering cross-sections of a perfectly conducting prolate spheroid... Fig. 3.6. Normalized differential scattering cross-sections of a perfectly conducting prolate spheroid...
Fig. 3.8. Variation of the normalized differential scattering cross-sections with the axial position of a prolate spheroid illuminated by a Gaussian beam... Fig. 3.8. Variation of the normalized differential scattering cross-sections with the axial position of a prolate spheroid illuminated by a Gaussian beam...
In Figs. 3.14-3.17 we plot the normalized differential scattering cross-sections together with the results computed with the discrete sources method for parallel and perpendicular polarizations, and for the case of normal incidence. It is apparent that the agreement between the curves is acceptable. [Pg.210]

Fig. 3.14. Normalized differential scattering cross-sections of a prolate spheroid with a = 8.5 pm and b = 0.85 pm. The curves are computed with the TAXSYM... Fig. 3.14. Normalized differential scattering cross-sections of a prolate spheroid with a = 8.5 pm and b = 0.85 pm. The curves are computed with the TAXSYM...
Fig. 3.16. Normalized differential scattering cross-sections of an oblate cylinder with a = 0.03 tm and b = 3.0 tm. The curves axe computed with the TAXSYM routine and the discrete sources method (DSM)... Fig. 3.16. Normalized differential scattering cross-sections of an oblate cylinder with a = 0.03 tm and b = 3.0 tm. The curves axe computed with the TAXSYM routine and the discrete sources method (DSM)...
Fig. 3.33. Normalized differential scattering cross-sections for perpendicular polarization of a cube and a reconstructed cube... Fig. 3.33. Normalized differential scattering cross-sections for perpendicular polarization of a cube and a reconstructed cube...
Fig. 3.36. Normalized differential scattering cross-sections of an inhomogeneous sphere with a spheroidal inclusion. The results are computed with the TINHOM routine and the multiple multipole method (MMP)... Fig. 3.36. Normalized differential scattering cross-sections of an inhomogeneous sphere with a spheroidal inclusion. The results are computed with the TINHOM routine and the multiple multipole method (MMP)...

See other pages where Differential scattering cross-section normalized is mentioned: [Pg.72]    [Pg.286]    [Pg.7]    [Pg.236]    [Pg.356]    [Pg.281]    [Pg.465]    [Pg.120]    [Pg.83]    [Pg.228]    [Pg.229]    [Pg.213]    [Pg.273]    [Pg.726]    [Pg.42]    [Pg.51]    [Pg.203]    [Pg.213]    [Pg.222]   
See also in sourсe #XX -- [ Pg.42 ]




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